he p - th / 9 80 81 58 26 A ug 1 99 8 UCL { IPT { 98 { 13 On Parity Functions in Conformal Field

ar X iv : 0 80 8 . 24 81 v 1 [ he p - th ] 1 8 A ug 2 00 8 MIFP - 08 - 21 USTC - ICTS - 08 - 14 AdS

We obtain a large class of smooth Lorentzian p-brane wormholes in supergravities in various dimensions. They connect two asymptotically flat spacetimes. In cases where there is no dilaton involved in the solution, the wormhole can connect an AdSn × Sm in one asymptotic region to a flat spacetime in the other. We obtain explicit examples for (n,m) = (4, 7), (7, 4), (5, 5), (3, 3), (3, 2). These ...

as tr o - ph / 9 80 81 94 19 A ug 1 99 8 Magnetic Field Effects on the Structure of Radiatively

- th / 9 70 80 13 v 1 8 A ug 1 99 7 Antisymmetry and channel coupling contributions to the absorption for p + α / d + 3

abstract: To understand recently established empirical p + α potentials, RGM calculations followed by inversion are made to study contributions of the d + 3 He reaction channels and deuteron distortion effects to the p + α potential. An equivalent study of the d + 3 He potential is also presented. The contributions of exchange non-locality to the absorption are simulated by including an phenome...

A Multivariate Sign EWMA Control Chart

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H EP - T H / 97 08 ∣ 0 6 * he p - th / 9 70 81 06 20 A ug 1 99 7

On the basis of the principle that topological quantum phases arise from the scattering around space-time defects in higher dimensional uniication, a geometric model is presented that associates with each quantum phase an element of a transformation group.